3.2)Show that, in a typical Ekman spiral solution with a constant verticaleddy viscosity A¸, the bottom stress 7,), if expressed in the complex formyB+ ityBcan be written as= T'BxBpfD,V.E4ewhere DE= T2A/f is the Ekman layer depth and V,=u. + iv.

3.2) Show that, in a typical Ekman spiral solution with a constant vertical eddy viscosity A¸, the bottom stress i, = (T. yB „T), if expressed in the complex form %3D T = TR +it yB can be written as B xB pfD, 'B V27 EV 4 %3D where D. = x /2A /f is the Ekman layer depth and V = u_ +iv_ .

3.2) Show that, in a typical Ekman spiral solution with a constant vertical eddy viscosity A¸, the bottom stress i, = (T. yB „T), if expressed in the complex form %3D T = TR +it yB can be written as B xB pfD, 'B V27 EV 4 %3D where D. = x /2A /f is the Ekman layer depth and V = u_ +iv_ .

Elements Of Electromagnetics

7th Edition

ISBN:9780190698614

Author:Sadiku, Matthew N. O.

Publisher:Sadiku, Matthew N. O.

ChapterMA: Math Assessment

Section: Chapter Questions

Problem 1.1MA

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